1,291 research outputs found

    Giant capacitance of a plane capacitor with a two-dimensional electron gas in a magnetic field

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    If a clean two-dimensional electron gas (2DEG) with small concentration nn comprises one (or both) electrodes of a plane capacitor, the resulting capacitance CC can be larger than the "geometric capacitance" CgC_g determined by the physical separation dd between electrodes. A recent paper [1] argued that when the effective Bohr radius aBa_B of the 2DEG satisfies aB<<da_B << d, one can achieve C>>CgC >> C_g at low concentration nd2<<1nd^2 << 1. Here we show that even for devices with aB>da_B > d, including graphene, for which aBa_B is effectively infinite, one also arrives at C>>CgC >> C_g at low electron concentration if there is a strong perpendicular magnetic field.Comment: 6 pages, 5 figures; updated discussion about bilayer systems; added discussion of fractional quantum Hall state

    Phenomenological Model of Vortex Generators

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    UnconstrainedMiner : efficient discovery of generalized declarative process models

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    Process discovery techniques derive a process model from observed behavior (e.g., event logs). In case of less structured processes, declarative models have notable advantages over procedural models. A declarative model consists of a set of temporal constraints over the activities in the event log. In this paper, we address three limitations of current discovery techniques: their unclear semantics of declarative constraints for business processes, their non-performative discovery of constraints, and their potential identification of vacuous constraints. We implemented our contributions as a declarative discovery algorithm for the Declare language. Our evaluations on a real-life event log indicate that it outperforms state of the art techniques by several orders of magnitude

    Det 17. aarhundredes adelige Ligprædikener og deres Kobberstik

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    Ultrastable lasers based on vibration insensitive cavities

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    We present two ultra-stable lasers based on two vibration insensitive cavity designs, one with vertical optical axis geometry, the other horizontal. Ultra-stable cavities are constructed with fused silica mirror substrates, shown to decrease the thermal noise limit, in order to improve the frequency stability over previous designs. Vibration sensitivity components measured are equal to or better than 1.5e-11 per m.s^-2 for each spatial direction, which shows significant improvement over previous studies. We have tested the very low dependence on the position of the cavity support points, in order to establish that our designs eliminate the need for fine tuning to achieve extremely low vibration sensitivity. Relative frequency measurements show that at least one of the stabilized lasers has a stability better than 5.6e-16 at 1 second, which is the best result obtained for this length of cavity.Comment: 8 pages 12 figure

    JEM-X background models

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    Background and determination of its components for the JEM-X X-ray telescope on INTEGRAL are discussed. A part of the first background observations by JEM-X are analysed and results are compared to predictions. The observations are based on extensive imaging of background near the Crab Nebula on revolution 41 of INTEGRAL. Total observing time used for the analysis was 216502 s, with the average of 25 cps of background for each of the two JEM-X telescopes. JEM-X1 showed slightly higher average background intensity than JEM-X2. The detectors were stable during the long exposures, and weak orbital phase dependence in the background outside radiation belts was observed. The analysis yielded an average of 5 cps for the diffuse background, and 20 cps for the instrument background. The instrument background was found highly dependent on position, both for spectral shape and intensity. Diffuse background was enhanced in the central area of a detector, and it decreased radially towards the edge, with a clear vignetting effect for both JEM-X units. The instrument background was weakest in the central area of a detector and showed a steep increase at the very edges of both JEM-X detectors, with significant difference in spatial signatures between JEM-X units. According to our modelling, instrument background dominates over diffuse background in all positions and for all energies of JEM-X.Comment: 4 pages, 3 figures, A&A accepted (INTEGRAL special issue
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